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From the lab to the real world: Sources of error in uranium hexafluoride gas enrichment monitoring.

机译:从实验室到现实世界:六氟化铀气体富集监测的误差来源。

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摘要

Safeguarding uranium enrichment facilities is a serious concern for the International Atomic Energy Agency (IAEA). Safeguards methods have changed over the years, most recently switching to an improved safeguards model that calls for new technologies to help keep up with the increasing size and complexity of today's gas centrifuge enrichment plants (GCEPs). One of the primary goals of the IAEA is to detect the production of uranium at levels greater than those an enrichment facility may have declared. In order to accomplish this goal, new enrichment monitors need to be as accurate as possible.;This dissertation will look at the Advanced Enrichment Monitor (AEM), a new enrichment monitor designed at Los Alamos National Laboratory. Specifically explored are various factors that could potentially contribute to errors in a final enrichment determination delivered by the AEM. There are many factors that can cause errors in the determination of uranium hexafluoride (UF 6) gas enrichment, especially during the period when the enrichment is being measured in an operating GCEP. To measure enrichment using the AEM, a passive 186-keV (kiloelectronvolt) measurement is used to determine the 235U content in the gas, and a transmission measurement or a gas pressure reading is used to determine the total uranium content. A transmission spectrum is generated using an x-ray tube and a "notch" filter.;In this dissertation, changes that could occur in the detection efficiency and the transmission errors that could result from variations in pipe-wall thickness will be explored. Additional factors that could contribute to errors in enrichment measurement will also be examined, including changes in the gas pressure, ambient and UF6 temperature, instrumental errors, and the effects of uranium deposits on the inside of the pipe walls will be considered. The sensitivity of the enrichment calculation to these various parameters will then be evaluated. Previously, UF6 gas enrichment monitors have required empty pipe measurements to accurately determine the pipe attenuation (the pipe attenuation is typically much larger than the attenuation in the gas). This dissertation reports on a method for determining the thickness of a pipe in a GCEP when obtaining an empty pipe measurement may not be feasible.;This dissertation studies each of the components that may add to the final error in the enrichment measurement, and the factors that were taken into account to mitigate these issues are also detailed and tested. The use of an x-ray generator as a transmission source and the attending stability issues are addressed. Both analytical calculations and experimental measurements have been used. For completeness, some real-world analysis results from the URENCO Capenhurst enrichment plant have been included, where the final enrichment error has remained well below 1% for approximately two months.
机译:维护铀浓缩设施是国际原子能机构(IAEA)的严重关切。多年来,保障方法已经发生了变化,最近切换到一种改进的保障模型,该模型要求使用新技术来帮助跟上当今气体离心浓缩厂(GCEP)不断增长的规模和复杂性。原子能机构的主要目标之一是检测铀的生产量,其水平高于浓缩设施可能宣布的水平。为了实现这个目标,新的浓缩监测仪需要尽可能的准确。本论文将研究高级浓缩监测仪(AEM),这是由洛斯阿拉莫斯国家实验室设计的一种新型的浓缩监测仪。专门探讨了各种因素,这些因素可能会导致AEM进行最终富集测定时出错。有很多因素会导致六氟化铀(UF 6)气体富集度测定中的错误,尤其是在运行的GCEP中测量富集度期间。为了使用AEM来测量浓缩,使用无源186keV(千伏)测量来确定气体中的235U含量,并使用透射率测量或气压读数来确定总铀含量。使用X射线管和“陷波”滤光片产生透射光谱。本文将探讨检测效率可能发生的变化以及由于管壁厚度的变化而引起的透射误差。还将检查可能导致浓缩测量误差的其他因素,包括气压,环境温度和UF6温度的变化,仪器误差以及将考虑铀沉积在管壁内部的影响。然后将评估浓缩计算对这些各种参数的敏感性。以前,UF6气体浓缩监测仪需要进行空管测量才能准确确定管道衰减(管道衰减通常比气体中的衰减大得多)。本论文报告了一种在获得空管测量值时确定GCEP中管子厚度的方法可能不可行的方法;该论文研究了可能会增加浓缩测量最终误差的每个成分以及影响因素减轻这些问题的考虑因素也得到了详细的测试。解决了使用X射线发生器作为传输源以及随之而来的稳定性问题。分析计算和实验测量均已使用。为了完整起见,URENCO Capenhurst浓缩厂的一些实际分析结果已包括在内,其中大约两个月的最终浓缩误差始终低于1%。

著录项

  • 作者

    Lombardi, Marcie L.;

  • 作者单位

    The University of New Mexico.;

  • 授予单位 The University of New Mexico.;
  • 学科 Engineering Chemical.;Engineering Nuclear.
  • 学位 Ph.D.
  • 年度 2012
  • 页码 154 p.
  • 总页数 154
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

  • 入库时间 2022-08-17 11:43:06

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